User:Sandbox/Du Bois-Reymond Constants/Example/First
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Example of Du Bois-Reymond Constant
The first du Bois-Reymond constant $C_1$ does not exist.
This is because:
- $\ds \int_0^\infty \size {\map {\dfrac \d {\d t} } {\dfrac {\sin t} t}^n} \rd t - 1$
does not converge for $n = 1$.
Proof
Let:
- $\ds \map f t = \frac{\sin t} t$
Its derivative is:
- $\ds \map {f'} t = \frac{t \map \cos t - \map \sin t}{t^2}$
Let $\ds \sequence {t_n}_{n \mathop = 1}^\infty$ be all the positive roots of $\map {f'} {t}$ in increasing order.
Equivalently, $\ds \sequence {t_n}_{n \mathop = 1}^\infty$ are all the positive roots of $t = \map \tan t$.
So:
\(\text {(1)}: \quad\) | \(\ds n \pi\) | \(<\) | \(\ds t_n\) | \(\ds < \frac {\pi} 2 + n \pi\) |
|
and:
\(\text {(2)}: \quad\) | \(\ds \size {\map \sin {t_n} }\) | \(\ge\) | \(\ds \size {\map \sin {t_1} }\) |
|
Since $\sequence {t_n}$ are roots of $f'$, the sign of $\map {f'} t$ alternates between positive and negative on each interval:
\(\ds \map {f'} t\) | \(<\) | \(\ds 0\) | for $0 < t < t_1$ | |||||||||||
\(\ds \map {f'} t\) | \(>\) | \(\ds 0\) | for $t_1 < t < t_2$ | |||||||||||
\(\ds \map {f'} t\) | \(<\) | \(\ds 0\) | for $t_2 < t < t_3$ | |||||||||||
\(\ds \map {f'} t\) | \(>\) | \(\ds 0\) | for $t_3 < t < t_4$ | |||||||||||
\(\ds \) | \(\vdots\) | \(\ds \) |
By definition of absolute value:
- $\size {\map {f'} t} = -\map {f'} t$ for $t \in \closedint 0 {t_1} \cup \closedint {t_2} {t_3} \cup \cdots$
- $\size {\map {f'} t} = \map {f'} t$ for $t \in \closedint {t_1} {t_2} \cup \closedint {t_3} {t_4} \cup \cdots$
\(\ds \size {\map {f'} t}\) | \(=\) | \(\ds -\map {f'} t\) | for $t \in \closedint 0 {t_1} \cup \closedint {t_2} {t_3} \cup \cdots$ | |||||||||||
\(\ds \size {\map {f'} t}\) | \(=\) | \(\ds \map {f'} t\) | for $t \in \closedint {t_1} {t_2} \cup \closedint {t_3} {t_4} \cup \cdots$ |
Also, by Fundamental Theorem of Calculus:
- $\ds \int_{t_n}^{t_{n + 1} } \map {f'} t \rd t = \map f {t_{n + 1} }- \map f {t_n}$
Substituting these into the integral:
\(\ds \ds \int_0^\infty \size {\map {f'} t} \rd t\) | \(=\) | \(\ds \int_0^{t_1} \size {\map {f'} t} \rd t + \int_{t_1}^{t_2} \size {\map {f'} t} \rd t + \cdots\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -\paren {\map f {t_1} - 0} + \paren {\map f {t_2}- \map f {t_1} } - \paren {\map f {t_3}- \map f {t_2} } + \paren {\map f {t_4}- \map f {t_3} } - \cdots\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds 2 \sum_{n \mathop = 1}^\infty \size {\map f {t_n} }\) | ||||||||||||
\(\text {(3)}: \quad\) | \(\ds \) | \(=\) | \(\ds 2 \sum_{n \mathop = 1}^\infty \frac{\size {\map \sin {t_n} } } {t_n}\) |
By $(1)$, we have:
- $t_n < \dfrac \pi 2 + n \pi$
By $(2)$, we have:
- $\size {\map \sin {t_1} } \le \size {\map \sin {t_n} }$
So:
- $\dfrac {\size {\map \sin {t_n} } } {t_n} > \dfrac {\size {\map \sin {t_1} } } {\dfrac \pi 2 + n \pi}$
But:
- $\ds \sum_{n \mathop = 1}^\infty \frac {\size {\map \sin {t_1} } } {\frac \pi 2 + n \pi} = \infty$
By Comparison Test for Divergence:
- $\ds \sum_{n \mathop = 1}^\infty \frac{\size {\map \sin {t_n} } }{t_n} = \infty$
By $(3)$, the integral diverges.
$\blacksquare$